Incline Plane Problem: Determining Velocity of a Mass at Height h1

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Homework Help Overview

The problem involves a mass sliding down a frictionless incline at an angle theta, starting from rest at a height of h(1) + h(2) and sliding off the ramp at height h(1). The original poster seeks to determine the velocity vector of the mass as it leaves the ramp.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster applies both force equations and mechanical energy equations to find the velocity, leading to different results. Some participants suggest focusing on the speed at the end of the ramp and ensuring the velocity components are properly aligned with the ramp.

Discussion Status

Participants are actively engaging with the original poster's attempts, providing guidance on refining the approach and suggesting the elimination of variables to simplify the expressions for comparison. There is an ongoing exploration of the relationships between the variables involved.

Contextual Notes

Participants note the need to express the velocity in vector form and question the assumptions made regarding the relationship between height and the ramp length. The original poster's methods yield conflicting results, prompting further investigation into the equations used.

Benzoate
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Homework Statement



A mass slides on a frictionless plane inclined at an angle theta from the horizontal. The mass starts from rest at a height h(1)+h(2) , then slides off the ramp at height h(1).

I will post the link so you can visualized the problem

http://courses.ncsu.edu/py411/lec/001/

What is the velocity vector of the mass when the mass is at height h1 (as the mass leaves the ramp?)


Homework Equations



Force equations , Mechanical Energy equations



The Attempt at a Solution



I apply to methods to determined the velocity of mass : Forces equations and Mechanical Energy equations. I will start with Force equations

y component: F(normal)-mg cos(theta)=0, nothing moves in y direction

x-components: mg sin(theta)-0=m*a=> a=g*sin(theta) ; next thing I did was integrate a to get v and now v = gt*sin(theta). My prof said he wanted my v in vector form, meaning I think he wants the velocity , in the x, y and z directions. so v= (gt sin(theta))x + (gt cos(theta)+0 z.

Now I will find the velocity the alternative way:

(K(f)-K(i))+(U(f)-U(i))=0=> ((.5*m*v^2)-0)+(0-m*g*h2))=0 +> v=sqrt(2*g*h2). Both methods lead me to different velocities. What did I do wrong?
 
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Benzoate said:
x-components: mg sin(theta)-0=m*a=> a=g*sin(theta) ; next thing I did was integrate a to get v and now v = gt*sin(theta).
You found the speed as a function of time (assuming it starts from rest). What you need is the speed at the end of the ramp. Keep going.

And note that that velocity will be parallel to the ramp, so find its components properly.
 
Doc Al said:
You found the speed as a function of time (assuming it starts from rest). What you need is the speed at the end of the ramp. Keep going.

And note that that velocity will be parallel to the ramp, so find its components properly.

should I continue to integrate the velocity vector to come up with the position vector? Now I have an equation that looks like this:

gt^2/2*sin(theta)=x, x being the length of the ramp I guess

gt^2/2*(h2/sqrt((h2)^2+x^2))=sqrt((h2)^2+x^2)) => t= sqrt(2*((h2)^2+x^2)/g*h2)) and now I can plug t into v=gt*sin(theta) right?
 
Right idea. But you want to eliminate x, so rewrite it in terms of h2 and theta. Then be sure to simplify the final expression, so you can compare it with your other solution.
 

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